EP3767683A1 - Transistor mit hoher elektronenbeweglichkeit und sein herstellungsverfahren - Google Patents

Transistor mit hoher elektronenbeweglichkeit und sein herstellungsverfahren Download PDF

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EP3767683A1
EP3767683A1 EP20168434.7A EP20168434A EP3767683A1 EP 3767683 A1 EP3767683 A1 EP 3767683A1 EP 20168434 A EP20168434 A EP 20168434A EP 3767683 A1 EP3767683 A1 EP 3767683A1
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Prior art keywords
layer
hemt
electron mobility
high electron
mobility transistor
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French (fr)
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Kuo-Hsing Lee
Yi-Chung Sheng
Sheng-Yuan Hsueh
Chih-Kai Kang
Guan-Kai Huang
Chien-Liang Wu
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United Microelectronics Corp
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United Microelectronics Corp
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    • H01L29/778Field effect transistors with two-dimensional charge carrier gas channel, e.g. HEMT ; with two-dimensional charge-carrier layer formed at a heterojunction interface
    • H01L29/7786Field effect transistors with two-dimensional charge carrier gas channel, e.g. HEMT ; with two-dimensional charge-carrier layer formed at a heterojunction interface with direct single heterostructure, i.e. with wide bandgap layer formed on top of active layer, e.g. direct single heterostructure MIS-like HEMT
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    • H01L29/66446Unipolar field-effect transistors with an active layer made of a group 13/15 material, e.g. group 13/15 velocity modulation transistor [VMT], group 13/15 negative resistance FET [NERFET]
    • H01L29/66462Unipolar field-effect transistors with an active layer made of a group 13/15 material, e.g. group 13/15 velocity modulation transistor [VMT], group 13/15 negative resistance FET [NERFET] with a heterojunction interface channel or gate, e.g. HFET, HIGFET, SISFET, HJFET, HEMT
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    • H01L29/42356Disposition, e.g. buried gate electrode
    • H01L29/4236Disposition, e.g. buried gate electrode within a trench, e.g. trench gate electrode, groove gate electrode

Definitions

  • the present invention relates to a high electron mobility transistor (HEMT) and forming method thereof, and more particularly, to a high electron mobility transistor (HEMT) electrically connecting a control gate to a source electrode and forming method thereof.
  • HEMT high electron mobility transistor
  • High electron mobility transistor has various advantages in electrical, mechanical, and chemical aspects of the field. For instance, advantages including wide band gap, high break down voltage, high electron mobility, high elastic modulus, high piezoelectric and piezoresistive coefficients, and chemical inertness. All of these advantages allow high electron mobility transistor (HEMT) to be used in numerous applications including high intensity light emitting diodes (LEDs), power switching devices, regulators, battery protectors, display panel drivers, and communication devices.
  • LEDs high intensity light emitting diodes
  • High electron mobility transistor is also a field effect transistor, which has a carrier channel formed from a heterojunction at the interface between layers having different bandgap.
  • Ternary compound semiconductors such as gallium arsenide or aluminium gallium arsenide may be utilized to constitute this kind of devices. Instead, other materials may be applied. For instance, indium containing devices have good performance in high frequencies.
  • Gallium nitride (GaN) high electron mobility transistors (HEMT) attract attention recently due to its good performance in high frequencies.
  • the present invention provides a high electron mobility transistor (HEMT) and forming method thereof, which electrically connects a control gate to a source electrode, to reduce voltage difference between a main gate and a drain electrode.
  • HEMT high electron mobility transistor
  • the present invention provides a high electron mobility transistor (HEMT) includes a carrier transit layer, a carrier supply layer, a main gate, a control gate, a source electrode and a drain electrode.
  • the carrier transit layer is on a substrate.
  • the carrier supply layer is on the carrier transit layer.
  • the main gate and the control gate are on the carrier supply layer.
  • the source electrode and the drain electrode are at two opposite sides of the main gate and the control gate, wherein the source electrode is electrically connected to the control gate by a metal interconnect.
  • the present invention provides a method of forming a high electron mobility transistor (HEMT) including the following steps.
  • a carrier transit layer and a carrier supply layer are sequentially formed on a substrate.
  • a main gate and a control gate are formed on the carrier supply layer.
  • a source electrode and a drain electrode are formed at two opposite sides of the main gate and the control gate. The source electrode is electrically connected to the control gate by a metal interconnect.
  • the present invention provides a high electron mobility transistor (HEMT) and forming method thereof, which forms a carrier transit layer and a carrier supply layer on a substrate sequentially; forms a main gate and a control gate on the carrier supply layer; forms a source electrode and a drain electrode at two opposite sides of the main gate and the control gate; and electrically connects the source electrode to the control gate by a metal interconnect. Since the control gate is located between the main gate and the drain electrode, and the control gate is electrically connected to the source electrode, voltage difference between the main gate and the drain electrode can be reduced.
  • HEMT high electron mobility transistor
  • FIG.1 schematically depicts a cross-sectional view of a high electron mobility transistor (HEMT) according to an embodiment of the present invention.
  • a substrate 110 is provided.
  • the substrate 110 may be a semiconductor substrate such as a silicon substrate, a silicon containing substrate, a III-V group-on-silicon (such as GaN-on-silicon) substrate, a silicon carbide substrate, an aluminum oxide substrate, a graphene-on-silicon substrate or a silicon-on-insulator (SOI) substrate.
  • the substrate 110 may be a single-layered substrate, a multi-layered substrate, a gradient substrate, or combination thereof.
  • a buffer layer 120 is formed on the substrate 110.
  • the buffer layer 120 may be a stacked III-V group semiconductor layer, wherein the lattice constant of the stacked III-V group semiconductor layer varies gradually from bottom to top.
  • the buffer layer 120 may be gallium nitride (GaN) or aluminum nitride (AlN), but it is not limited thereto.
  • the buffer layer 120 may be formed by a molecular-beam epitaxy (MBE) process, a metal organic chemical vapor deposition (MOCVD) process, a chemical vapor deposition (CVD) process, a hydride vapor phase epitaxy (HVPE) process, or combination thereof.
  • MBE molecular-beam epitaxy
  • MOCVD metal organic chemical vapor deposition
  • CVD chemical vapor deposition
  • HVPE hydride vapor phase epitaxy
  • a carrier transit layer 130 is formed on the buffer layer 120.
  • the carrier transit layer 130 may be a stacked III-V group semiconductor layer, but it is not limited thereto.
  • the carrier transit layer 130 may be an unintentionally doped (UID) gallium nitride (GaN) layer.
  • the carrier transit layer 130 may be formed by a molecular-beam epitaxy (MBE) process, a metal organic chemical vapor deposition (MOCVD) process, a chemical vapor deposition (CVD) process, a hydride vapor phase epitaxy (HVPE) process, or combination thereof.
  • MBE molecular-beam epitaxy
  • MOCVD metal organic chemical vapor deposition
  • CVD chemical vapor deposition
  • HVPE hydride vapor phase epitaxy
  • a carrier supply layer 140 is formed on the carrier transit layer 130, thereby a channel region D1 being formed at an interface of the carrier transit layer 130 and the carrier supply layer 140.
  • the channel region D1 is the region where conductive current is formed by the two-dimensional electron gas (2DEG) and in such condition the HEMT device is typically operated under a "normally on” mode.
  • 2DEG two-dimensional electron gas
  • a heterojunction is formed at the interface between the carrier transit layer 130 and carrier supply layer 140 as a result of the bandgap difference between the two layers 130, 140.
  • a quantum well is formed in the banding portion of the conduction band of the heterojunction to constrain the electrons generated by piezoelectricity so that two-dimensional electron gas (2DEG) is formed at the junction between the carrier transit layer 130 and carrier supply layer 140 to form conductive current.
  • 2DEG two-dimensional electron gas
  • the carrier supply layer 140 may be a III-V group semiconductor layer, but it is not limited thereto.
  • the carrier supply layer 140 may be an unintentionally doped (UID) Al x Ga 1-x N layer, an n-type Al x Ga 1-x N layer or a p-type Al y Ga 1-y N layer.
  • the carrier supply layer 140 may be formed by an epitaxial growth process, which may include silicon or germanium etc.
  • the carrier supply layer 140 may be formed by a molecular-beam epitaxy (MBE) process, a metal organic chemical vapor deposition (MOCVD) process, a chemical vapor deposition (CVD) process, a hydride vapor phase epitaxy (HVPE) process, or combination thereof.
  • MBE molecular-beam epitaxy
  • MOCVD metal organic chemical vapor deposition
  • CVD chemical vapor deposition
  • HVPE hydride vapor phase epitaxy
  • a main gate 150 and a control gate 160 are formed on the carrier supply layer 140.
  • the main gate 150 may include a bottom part 152 and a top part 154, wherein the bottom part 152 and the top part 154 preferably include different materials.
  • the bottom part 152 may be a p-type Al y Ga 1-y N layer while the top part 154 may be metals or metal alloys such as gold, tungsten, cobalt, titanium, titanium nitride, molybdenum, copper, aluminum, ruthenium, palladium, silver or platinum or etc.
  • the control gate 160 may be metals or metal alloys such as gold, tungsten, cobalt, titanium, titanium nitride, molybdenum, copper, aluminum, ruthenium, palladium, silver or platinum or etc.
  • metals or metal alloys such as gold, tungsten, cobalt, titanium, titanium nitride, molybdenum, copper, aluminum, ruthenium, palladium, silver or platinum or etc.
  • As current gate electrodes typically made of metal gradually imports material such as p-type gallium nitride (GaN) to serve as bottom portion for the gate electrode, the operation of HEMT devices under this circumstance now shifts from “normally on” to "normally off”.
  • control gate 160 may only include metals or metal alloys, and the metals or the metal alloys directly contact the carrier supply layer 140.
  • a control gate 260 may include a bottom part 262 and a top part 264.
  • the bottom part 262 may be an insulating layer, which may include aluminum nitride, silicon nitride, aluminum oxide, or combination thereof, and the top part 264 may be metals or metal alloys such as gold, tungsten, cobalt, titanium, titanium nitride, molybdenum, copper, aluminum, tantalum, palladium, silver, platinum or etc.
  • the steps of forming the main gate 150 and the control gate 160/260 on the carrier supply layer 140 may include the following, but it is not limited thereto.
  • the bottom part 152 (being a P-type gallium nitride (GaN) layer in this embodiment) is formed on a part of the carrier supply layer 140 (the region for forming the main gate 150), which may include the following.
  • a P-type gallium nitride (GaN) layer is deposited blanketly and then patterned to form the P-type gallium nitride (GaN) layer on the part of the carrier supply layer 140.
  • a blanket interdielectric layer 170' is formed to blanketly cover the carrier supply layer 140 and the bottom part 152.
  • the blanket interdielectric layer 170' is patterned to form an interdielectric layer 170, as shown in FIG.4 .
  • the interdielectric layer 170 include a main gate recess R1 and a control gate recess R2, wherein the main gate recess R1 exposes the bottom part 152, and the control gate recess R2 exposes the carrier supply layer 140.
  • a metal gate is directly formed on the bottom part 152 in the main gate recess R1 for serving as the top part 154 of the main gate 150, and a metal gate is directly formed on the carrier supply layer 140 in the control gate recess R2 for serving as the control gate 160.
  • the metal gate used for forming the top part 154 and the metal gate used for forming the control gate 160 may have common or different materials, and the metal gates are formed at a same time or are formed respectively, depending upon practical requirements.
  • the bottom part 262 (being an insulating layer in this embodiment) is formed on the carrier supply layer 140 in the control gate recess R2, and then metal gates are directly formed on the bottom part 152 in the main gate recess R1, and on the bottom part 262 in the control gate recess R2 respectively, wherein the metal gate in the main gate recess R1 serves as the top part 154 of the main gate 150, and the metal gate in the control gate recess R2 serves as the top part 264 of the control gate 260.
  • the metal gate used for forming the top part 154 and the metal gate used for forming the top part 264 may have common or different materials, and the metal gates are formed at a same time or are formed respectively, depending upon practical requirements.
  • a source electrode 182 and a drain electrode 184 are formed at two opposite sides of the main gate 150 and the control gate 160.
  • Methods of forming the source electrode 182 and the drain electrode 184 at the two opposite sides of the main gate 150 and the control gate 160 may include the following.
  • the carrier supply layer 140 is etched to form a source recess R3 and a drain recess R4 in the carrier supply layer 140 at the two opposite sides of the main gate 150 and the control gate 160.
  • the source electrode 182 is formed in the source recess R3 and the drain electrode 184 is formed in the drain recess R4.
  • a bottom surface S1 of the source electrode 182, a bottom surface S2 of the drain electrode 184 and a bottom surface S3 of the carrier supply layer 140 are coplanar, to directly contact a channel region D1/D2 (meaning a two-dimensional electron gas (2DEG) channel) at an interface of the carrier transit layer 130 and the carrier supply layer 140.
  • the source electrode 182 and the drain electrode 184 may be metals or metal alloys such as gold, tungsten, cobalt, titanium, titanium nitride, molybdenum, copper, aluminum, tantalum, palladium, silver or platinum or etc.
  • the source electrode 182 is electrically connected to the control gate 160/260 by a metal interconnect 190.
  • the metal interconnect 190 may be formed by a dual damascene process or a single damascene process etc, wherein the metal interconnect 190 may be a metal line disposed over but without contacting the main gate 150, and the metal interconnect 190 directly contacts the source electrode 182 to the control gate 160/260, but it is not limited thereto. Therefore, a high electron mobility transistor (HEMT) 100/200 is formed.
  • HEMT high electron mobility transistor
  • control gate 160/260 being formed between the main gate 150 and the drain electrode 184, and the metal interconnect 190 electrically connects the source electrode 182 to the control gate 160/260
  • voltage difference between the main gate 150 and the drain electrode 184 can be reduced while the device of the present invention turns off.
  • the voltage difference between the main gate 150 and the drain electrode 184 can decrease to 200-300 volts from 600 volts by using the control gate 160/260.
  • FIG.7 schematically depicts a cross-sectional view of a high electron mobility transistor (HEMT) 300 including a main gate doped with fluorine according to another embodiment of the present invention.
  • the main gate 350 may be composed of metals or metal alloys such as gold, tungsten, cobalt, titanium, titanium nitride, molybdenum, copper, aluminum, tantalum, palladium, silver, platinum or etc, but it is not limited thereto.
  • fluorine is doped in the carrier supply layer 140 right below the main gate 350, thereby forming a fluoride ion doped region 10 right below the main gate 350, wherein the step of doping fluorine may be processed after the main gate 350 and the control gate 260 are formed, and before the source electrode 182 and the drain electrode 184 are formed, but it is not limited thereto.
  • a bottom part of the main gate 350 may include an insulating layer 352 directly on the fluoride ion doped region 10.
  • the insulating layer 352 may include a stacked layer constituted by aluminum nitride, silicon nitride, aluminum oxide or etc.
  • the insulating layer 352 and the bottom part 262 (, which is also an insulating layer) of the control gate 260 have common thicknesses. In other cases, a thickness of the insulating layer 352 is less than a thickness of the bottom part 262, depending upon practical requirements.
  • the insulating layer 352 and the bottom part 262 of the control gate 260 are formed at a same time or are formed respectively. Thus, the voltage difference between the main gate 350 and the drain electrode 184 can be reduced while the high electron mobility transistor (HEMT) 300 turns off.
  • HEMT high electron mobility transistor
  • FIG.8 schematically depicts a cross-sectional view of a high electron mobility transistor (HEMT) 400 including a recessed main gate according to another embodiment of the present invention.
  • HEMT high electron mobility transistor
  • the main gate 450 may be composed of metals or metal alloys such as gold, tungsten, cobalt, titanium, titanium nitride, molybdenum, copper, aluminum, tantalum, palladium, silver, platinum or etc, but it is not limited thereto.
  • a recess R5 is formed in the carrier supply layer 140, and then the main gate 450 is formed in the carrier supply layer 140, thereby the recessed main gate 450 being formed, but it is not limited thereto.
  • a bottom part of the main gate 450 may include an insulating layer 452 directly on the carrier supply layer 140.
  • the insulating layer 452 may include a stacked layer constituted by aluminum nitride, silicon nitride, aluminum oxide or etc.
  • the insulating layer 452 and the bottom part 262 (, which is also an insulating layer) of the control gate 260 have common thicknesses.
  • a thickness of the insulating layer 452 is less than a thickness of the bottom part 262 of the control gate 260, depending upon practical requirements.
  • the insulating layer 452 and the bottom part 262 of the control gate 260 are formed at a same time or are formed respectively.
  • the voltage difference between the main gate 450 and the drain electrode 184 can be reduced while the high electron mobility transistor (HEMT) 400 turns off.
  • HEMT high electron mobility transistor
  • the present invention provides a high electron mobility transistor (HEMT) and forming method thereof, which forms a carrier transit layer and a carrier supply layer on a substrate sequentially; forms a main gate and a control gate on the carrier supply layer; forms a source electrode and a drain electrode at two opposite sides of the main gate and the control gate; and electrically connects the source electrode to the control gate by a metal interconnect. Since the control gate is located between the main gate and the drain electrode, and the control gate is electrically connected to the source electrode, the voltage difference between the main gate and the drain electrode can be reduced.
  • HEMT high electron mobility transistor
  • HEMT high electron mobility transistor
  • a high electron mobility transistor (HEMT) including a P-type Al x Ga 1-x N main gate a high electron mobility transistor (HEMT) including a fluorine doped main gate or a high electron mobility transistor (HEMT) including a recessed main gate.
  • Insulating layers are selectively formed in bottom parts of the main gate and the control gate, and relative thicknesses of the insulating layers of the main gate and the control gate depend upon practical requirements.

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  • Junction Field-Effect Transistors (AREA)
EP20168434.7A 2019-07-18 2020-04-07 Transistor mit hoher elektronenbeweglichkeit und sein herstellungsverfahren Pending EP3767683A1 (de)

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CN115483197A (zh) 2021-05-31 2022-12-16 联华电子股份有限公司 电容器结构以及其制作方法
CN115966466A (zh) 2021-10-12 2023-04-14 联华电子股份有限公司 高电子迁移率晶体管及其制作方法
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